Electromagnetic Induction
and Alternating Current
Magnetic
Flux
The
magnetic flux is proportional to the number of
field
lines that pass through the surface.
Φ
=
Bn
A
Φ
magnetic flux in Wb (Weber). Also
: T.m2 of Vs
Bn
the component of B perpendicular to the
surface in T(esla)
A
area of the surface in m2
Example
See the
drawing above.
B = 1.5
x 10-3
T
A = 500
cm2
α
= 40
o
Resolve
B in both components and calculate Bn
sin
α
= Bn/B
Bn = B sin 40
o
= (1.5 x 10-3
)( 0.643) = 9.642
x 10-4
T
Φ
= Bn
A
Φ
= (9.642 x 10-4
)( 500 x 10-4
)= 4.82 x 10-5 Wb
Change of magnetic flux and
electromagnetic induction
A change in the magnetic flux in a
closed circuit (coil)
induces
a potential difference .
Law of
Faraday:
Vind
average
induced potential difference in V
N
amount of loops of the coil
ΔΦ
change of magnetic flux in Wb
Δ
t time interval in
which change occurs in s
Example
See the
figure alongside.
The
area of the turn is 40 cm2
The
magnitude of the magnetic induction is
0.020 T
The turn is rotated.
At the
moment of the figure the field lines are parallel to
the turn.
So the
magnetic flux is 0 Wb
After
0.0050 s the turn has rotated 90o
. In that situation the magnetic
flux is maximal
Determine the average induced potential difference (emf) in this time interval.
Vind =-
N ( ΔΦ/Δt)
ΔΦ
= Φmax – 0 = B A = (0.020 )(40 x 10-4) = 8.0 x 10-5
Wb
Vind
= (1) (8.0 x 10-5)/0.0050
= 1.6 x 10-2 V
An induction
current is produced when A is connected to B
The resistance of
the circuit is 0.20
Ω
Uind = Iind
R
1.6 x 10-2 = (Iind )(0,20)
Iind
= 8,0.10-2 A
Sinusoidal
alternating current
Peak voltage and
root mean square value of voltage
V(t) = V0 sin
(2πft)
(set calculator to radians)
V voltage in
V
V 0
peak
voltage in V
f
frequency in Hz
t
time in s
Vrms = ½
√2 V
0
Vrms
root-mean-square
value of
voltage
Example 1
In the drawing
aside:
V 0 =10 V
T = 50 ms
f = 1/T=1/(50 x 10-3)
= 20 Hz
So :
V(t) = 10 sin (2π
20 t)
Vrms = ½
√2. V0
= ½ √2.
10 = 7.0 V
This means :
A DC voltage of
7.0 V produced the same power as an AC
voltage with a peak voltage of
10.0 V
Example 2
The mains voltage is :
V =230 V (This means :
V rms = 230 V)
Find the peak voltage.
Vrms = ½
√2
V 0
230 = ½
√2
V 0
V 0 = 325 V
Peak current and
root-mean-square value of the current
In the
previous paragraph we see : V(t) = V0
sin (2πft)
Correspondingly we can write for
the current:
I(t) = I 0 sin (2πft)
I rms =
½ √2.
I0
Transformer
VP
:
VS = NP
: NS
VP voltage
across the primary coil in V
VS voltage
induced in the secondary coil in V
NP
amount of turns in the primary coil
NS
amount of turns in the secondary coil
PP = PS
(Assuming
100 % energy transfer, no energy dissipated in heating))
VP IP
= VS IS
PP
power of the primary coil W (of
VA)
IP
current
in the primary coil in A
PS
power of the secondary coil
in W (of VA)
IS
current in the
secondary coil in A
Examples
1.
The
primary coil of a transformer consists of 400 turns. The secondary coil
80 turns.
The voltage across the primary coil is 230 V
Find the voltage across the secondary coil
VP
:
VS
= NP
: NS
230 : VS = 400 : 80
230 : VS = 5 : 1
(5)(Vs) = (230) (1
VS = 230/5 = 46 V
2.
The
primary coil is connected with an AC source
A bulb is connected with the
secondary coil.
The voltage across the bulb is
6.0 V and
the current through the bulb
is 0.4 A
The turns ratio is 5:1
(NP : NS
= 5: 1)
Calculate the current in the
primary coil
PS = VS
IS
= (6.0) (0.4) = 2.4 W
VP = 5 VS =
(5) (6.0) = 30
V
PP
= PS
= 2.4 W
PP
= VP
IP
2.4 = (30)( IP
IP = 2.4/30 = 0.8 A